“…Thermospheric winds at high latitudes are driven primarily by the ion drag associated with momentum transfer from the convecting plasma, Coriolis force, and pressure gradients caused by nonuniform temperature distributions due to solar radiative heating, Joule heating, and auroral particle precipitation (Killeen & Roble, 1988; Meriwether et al., 1973; Richmond et al., 2003; Roble et al., 1982; Tan et al., 2022; Wang & Luhr, 2016; Zhang et al., 2023). Driven by solar radiation‐produced pressure gradient force and the ion drag force associated with the convection pattern (Dungey, 1961), one of the large‐scale structures of the polar thermospheric wind is the anti‐sunward flow across the pole in the midnight sector, which is referred to as the “cross‐polar jet” (Smith et al., 1988, 1998).…”